PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK

An X5.4 class flare occurred in active region NOAA11429 on 2012 March 7. The flare was associated with a very fast coronal mass ejection (CME) with a velocity of over 2500 km s[−1]. In the images taken with the Solar Terrestrial Relations Observatory-B/COR1, a dome-like disturbance was seen to detac...

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Main Authors: Takahashi, Takuya, Asai, Ayumi, Shibata, Kazunari
Other Authors: 高橋, 卓也
Format: Article in Journal/Newspaper
Language:English
Published: American Astronomical Society 2015
Subjects:
Online Access:http://hdl.handle.net/2433/198606
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author Takahashi, Takuya
Asai, Ayumi
Shibata, Kazunari
author2 高橋, 卓也
author_facet Takahashi, Takuya
Asai, Ayumi
Shibata, Kazunari
author_sort Takahashi, Takuya
collection Kyoto University Research Information Repository (KURENAI)
description An X5.4 class flare occurred in active region NOAA11429 on 2012 March 7. The flare was associated with a very fast coronal mass ejection (CME) with a velocity of over 2500 km s[−1]. In the images taken with the Solar Terrestrial Relations Observatory-B/COR1, a dome-like disturbance was seen to detach from an expanding CME bubble and propagated further. A Type-II radio burst was also observed at the same time. On the other hand, in extreme ultraviolet images obtained by the Solar Dynamic Observatory/Atmospheric Imaging Assembly (AIA), the expanding dome-like structure and its footprint propagating to the north were observed. The footprint propagated with an average speed of about 670 km s[−1] and hit a prominence located at the north pole and activated it. During the activation, the prominence was strongly brightened. On the basis of some observational evidence, we concluded that the footprint in AIA images and the ones in COR1 images are the same, that is, the MHD fast mode shock front. With the help of a linear theory, the fast mode Mach number of the coronal shock is estimated to be between 1.11 and 1.29 using the initial velocity of the activated prominence. Also, the plasma compression ratio of the shock is enhanced to be between 1.18 and 2.11 in the prominence material, which we consider to be the reason for the strong brightening of the activated prominence. The applicability of linear theory to the shock problem is tested with a nonlinear MHD simulation.
format Article in Journal/Newspaper
genre North Pole
genre_facet North Pole
geographic North Pole
geographic_facet North Pole
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op_relation 10.1088/0004-637X/801/1/37
0004-637X
http://hdl.handle.net/2433/198606
AA00553242
The Astrophysical Journal
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op_rights © 2015. The American Astronomical Society.
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publisher American Astronomical Society
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spelling ftkyotouniv:oai:repository.kulib.kyoto-u.ac.jp:2433/198606 2025-01-16T23:48:54+00:00 PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK Takahashi, Takuya Asai, Ayumi Shibata, Kazunari 高橋, 卓也 2015-02-27 application/pdf http://hdl.handle.net/2433/198606 eng eng American Astronomical Society 10.1088/0004-637X/801/1/37 0004-637X http://hdl.handle.net/2433/198606 AA00553242 The Astrophysical Journal 801 1 37 © 2015. The American Astronomical Society. magnetohydrodynamics (MHD) shock waves Sun: corona Sun: filaments prominences Sun: flares Journal Article 2015 ftkyotouniv 2017-10-28T22:52:57Z An X5.4 class flare occurred in active region NOAA11429 on 2012 March 7. The flare was associated with a very fast coronal mass ejection (CME) with a velocity of over 2500 km s[−1]. In the images taken with the Solar Terrestrial Relations Observatory-B/COR1, a dome-like disturbance was seen to detach from an expanding CME bubble and propagated further. A Type-II radio burst was also observed at the same time. On the other hand, in extreme ultraviolet images obtained by the Solar Dynamic Observatory/Atmospheric Imaging Assembly (AIA), the expanding dome-like structure and its footprint propagating to the north were observed. The footprint propagated with an average speed of about 670 km s[−1] and hit a prominence located at the north pole and activated it. During the activation, the prominence was strongly brightened. On the basis of some observational evidence, we concluded that the footprint in AIA images and the ones in COR1 images are the same, that is, the MHD fast mode shock front. With the help of a linear theory, the fast mode Mach number of the coronal shock is estimated to be between 1.11 and 1.29 using the initial velocity of the activated prominence. Also, the plasma compression ratio of the shock is enhanced to be between 1.18 and 2.11 in the prominence material, which we consider to be the reason for the strong brightening of the activated prominence. The applicability of linear theory to the shock problem is tested with a nonlinear MHD simulation. Article in Journal/Newspaper North Pole Kyoto University Research Information Repository (KURENAI) North Pole
spellingShingle magnetohydrodynamics (MHD)
shock waves
Sun: corona
Sun: filaments
prominences
Sun: flares
Takahashi, Takuya
Asai, Ayumi
Shibata, Kazunari
PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title_full PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title_fullStr PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title_full_unstemmed PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title_short PROMINENCE ACTIVATION BY CORONAL FAST MODE SHOCK
title_sort prominence activation by coronal fast mode shock
topic magnetohydrodynamics (MHD)
shock waves
Sun: corona
Sun: filaments
prominences
Sun: flares
topic_facet magnetohydrodynamics (MHD)
shock waves
Sun: corona
Sun: filaments
prominences
Sun: flares
url http://hdl.handle.net/2433/198606